Conservation of Linear Momentum and Covariance

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SUMMARY

The discussion centers on the conservation of linear momentum in inelastic collisions, specifically analyzing two masses, m1' and m2', moving with velocities v1' and v2' in frame S' before colliding and sticking together to move with velocity v' in frame S. The Galilean transformation is utilized to relate the coordinates and velocities between the two frames, emphasizing that if momentum is conserved in S', it is also conserved in S. Key equations include the conservation of momentum equation m1v1 + m2v2 = (m1 + m2)vf and the linear momentum definition p = mv.

PREREQUISITES
  • Understanding of Galilean transformations
  • Knowledge of conservation of momentum in inelastic collisions
  • Familiarity with derivatives and their application in physics
  • Basic concepts of linear momentum
NEXT STEPS
  • Study the derivation of velocity transformations using Galilean transformations
  • Explore examples of inelastic collisions in different reference frames
  • Learn about the implications of momentum conservation in various physical scenarios
  • Investigate the differences between elastic and inelastic collisions
USEFUL FOR

Students of physics, educators teaching mechanics, and anyone interested in understanding the principles of momentum conservation and reference frame transformations.

Cave Johnson

Homework Statement


Assume two masses m1' and m2' are moving in the positive x-direction with velocities v1' and v2' as measured by an observer in S' before a collision. After the collision, the two masses stick together and move with velocity v' in S'. Show that if an observer in S' finds momentum conserved, so does an observer in S.

Homework Equations


Galilean Transformation:
x' = x - vt
y' = y
z' = z
t' = t

Conservation of momentum in inelastic collisions:
m1v1 + m2v2 = (m1 + m2)vf

Linear momentum:
p = mv

The Attempt at a Solution


I know that this will involve the use of this part of the GT:
x' = x - vt

I am confused on how to incorporate the conservation of momentum equation(s) into this, however.

Any help would be appreciated.
 
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How would you transform the velocities?
 
Doc Al said:
How would you transform the velocities?

I am not sure. I don't quite understand how to use these transformations for anything other than coordinates (like measuring lengths). I try to find examples in my textbook or online but they are all very confusing or blocked by a pay wall...
 
Cave Johnson said:
I don't quite understand how to use these transformations for anything other than coordinates (like measuring lengths).
Given the coordinate transformations, you can derive the velocity transformations by taking the derivative with respect to time. (It's easy!)
 
Doc Al said:
Given the coordinate transformations, you can derive the velocity transformations by taking the derivative with respect to time. (It's easy!)

Wouldn't that just leave us with -v ?
 
Cave Johnson said:
Wouldn't that just leave us with -v ?
Nope. Write the x-coordinate transform and take the derivative of each term.
 
Doc Al said:
Nope. Write the x-coordinate transform and take the derivative of each term.

Taking the derivative of x - vt with respect to time gives -v...
d/dt x = 0
d/dt -vt = -v
 
Cave Johnson said:
Taking the derivative of x - vt with respect to time gives -v...
d/dt x = 0
d/dt -vt = -v
Careful! The derivative of x with respect to t is not zero. It's dx/dt, which is a velocity measured in the S frame. Try it once more.
 

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